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arxiv: 2511.08014 · v2 · submitted 2025-11-11 · ⚛️ physics.flu-dyn

A Comprehensive Regime Diagram of Dynamical Modes of Triple Flickering Buoyant Diffusion Flames: Experimental and Model Investigations

Pith reviewed 2026-05-18 00:03 UTC · model grok-4.3

classification ⚛️ physics.flu-dyn
keywords triple flickering flamesbuoyant diffusion flamesdynamical modesregime diagramStuart-Landau oscillatortime-delay couplingsynchronizationbifurcation
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The pith

Moving one flame continuously maps out synchronization modes among three flickering buoyant flames.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The study examines three flickering laminar buoyant diffusion flames placed in an isosceles triangle to understand how they couple and synchronize. By moving the vertex flame at controlled speeds while independently changing the base length and fuel flow rate, the authors bypass the constraints of fixed discrete positions and generate a dense map of observed behaviors. This produces a regime diagram that classifies the dynamical modes and identifies three previously unreported modes. A model treating each flame as a Stuart-Landau oscillator with time-delay coupling reproduces the experimental patterns and links them to bifurcations in the coupled system. The work matters for anyone designing or analyzing arrays of flames, because the same coupling mechanisms appear in larger burners and can influence stability.

Core claim

Based on experimental observations, a comprehensive regime diagram was established to classify the dynamical modes of triple flickering buoyant diffusion flames. Notably, three previously unreported dynamical modes were identified for the first time. A Stuart-Landau oscillator model with time-delay coupling was employed, which successfully reproduces the experimentally observed dynamical modes. Experimentally observed dynamical modes reveal a bifurcation diagram for the coupled triple Stuart-Landau system.

What carries the argument

Stuart-Landau oscillator model with time-delay coupling, used to represent each flame's flickering amplitude and phase with delays that encode interaction times between the three flames.

If this is right

  • The regime diagram organizes observed modes according to triangle size, fuel flow rate, and vertex movement velocity.
  • Three new dynamical modes expand the catalog of possible synchronization states in triple flame systems.
  • The time-delay Stuart-Landau model reproduces the transitions between modes without solving the full fluid equations.
  • The experimental modes correspond directly to bifurcations in the coupled triple Stuart-Landau system.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The continuous-variation technique could be applied to other multi-flame geometries to discover additional modes without exhaustive static testing.
  • If the delayed-oscillator model scales, it offers a low-cost way to forecast stability limits in larger flame arrays used in industrial burners.
  • The same coupling framework might describe interactions in non-flame oscillator systems, such as groups of vortex wakes or acoustic resonators.

Load-bearing premise

That continuously moving the vertex flame at controlled speed produces dynamical modes equivalent to those found in static fixed-position configurations at matching effective parameters.

What would settle it

Performing a separate set of experiments with the three flames held completely fixed at discrete positions corresponding to the same L and Q values and checking whether the same sequence of modes appears as the vertex flame is stepped through those positions.

Figures

Figures reproduced from arXiv: 2511.08014 by Hanxu Wang, Peng Zhang, Tao Yang, Yicheng Chi, Zhenyu Zhang.

Figure 7
Figure 7. Figure 7: Phase trajectories of six typical dynamical modes in the triple flame system from [PITH_FULL_IMAGE:figures/full_fig_p017_7.png] view at source ↗
Figure 12
Figure 12. Figure 12: Mode IV-2: asymmetric partially in-phase mode reproduced by the Stuart￾Landau model. (a) Phase difference of three S-L oscillators (𝐾 = 0.25 , 𝜏1 = 2.20 , 𝜏2 = 3.40). (b) All model parameters of 𝐾, 𝜏1, and 𝜏2 for Mode IV-2 in the ranges of −0.5 < 𝐾 < 0.5 and 0 < 𝜏1, 𝜏2 < 5 [PITH_FULL_IMAGE:figures/full_fig_p021_12.png] view at source ↗
read the original abstract

The triple-flame system serves as the fundamental unit for understanding multi-flame interactions, revealing critical coupling mechanisms that scale to complex burner arrays. In this study, we investigated triple flame oscillators, consisting of three flickering laminar buoyant diffusion flames arranged in an isosceles triangular configuration, to construct a comparative regime diagram of dynamical modes. To overcome the limited experimental observability caused by the discretization of geometric parameters, we enabled continuous motion of the vertex flame at a controlled speed V, while independently varying the base length L and the fuel flow rate Q. We conducted a systematic investigation of the triple flame coupling behaviors by varying the triangle size, fuel flow rate, and vertex flame movement velocity. Based on the experimental observations, a comprehensive regime diagram was established to classify the dynamical modes of triple flickering buoyant diffusion flames. Notably, three previously unreported dynamical modes were identified for the first time. To interpret these complex flame interactions, a Stuart-Landau oscillator model with time-delay coupling was employed, which successfully reproduces the experimentally observed dynamical modes. Experimentally observed dynamical modes reveal a bifurcation diagram for the coupled triple Stuart-Landau system, elucidating the transitions between different synchronization modes.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript reports an experimental study of dynamical modes in three flickering buoyant diffusion flames arranged in an isosceles triangular geometry. By continuously translating the vertex flame at controlled speed V while varying base length L and fuel flow rate Q, the authors construct a regime diagram that classifies observed synchronization states, including three previously unreported modes. A Stuart-Landau oscillator model with time-delay coupling is employed to reproduce the modes and to map the associated bifurcation diagram for the coupled triple-oscillator system.

Significance. If the continuous-sweep method is shown to be dynamically equivalent to static configurations, the work would deliver a valuable comprehensive regime diagram for triple-flame interactions together with a reduced-order model that captures the observed bifurcations. The systematic exploration and identification of new modes constitute a concrete advance for understanding multi-flame coupling. The modeling effort is credited for providing an explicit bifurcation diagram, although its predictive status depends on how the coupling parameters were obtained.

major comments (2)
  1. [Experimental procedure for varying triangle size] The regime diagram and the three new modes rest on continuous variation of L achieved by moving the vertex flame at finite speed V. The manuscript provides no systematic test that the observed synchronization states remain unchanged for sufficiently small V, nor does it report the ratio of the natural flickering period to the time required to traverse one characteristic length at speed V. If this ratio is not ≪ 1, the sweep introduces advective and phase-lag effects absent from static isosceles triangles, rendering the reported boundaries and new modes potentially non-reproducible in fixed-geometry experiments.
  2. [Modeling section] The Stuart-Landau model with time-delay coupling is reported to reproduce the experimentally observed modes and to yield the bifurcation diagram. It is not stated whether the coupling strengths and delays were fixed from independent physical estimates or adjusted to match the target data set. Without this information the reproduction may be post-hoc rather than predictive, weakening the claim that the model elucidates the transitions between synchronization modes.
minor comments (2)
  1. [Abstract] The abstract states that a 'comprehensive regime diagram' was established but does not indicate the explored ranges of L, Q and V or the quantitative criteria used to assign a given trajectory to a particular mode.
  2. [Figures and captions] Figure captions and the regime diagram itself would benefit from explicit indication of the number of independent realizations and any uncertainty in the reported mode boundaries.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive review. The comments have prompted us to clarify key aspects of our experimental and modeling approaches. Below we respond point by point to the major comments.

read point-by-point responses
  1. Referee: [Experimental procedure for varying triangle size] The regime diagram and the three new modes rest on continuous variation of L achieved by moving the vertex flame at finite speed V. The manuscript provides no systematic test that the observed synchronization states remain unchanged for sufficiently small V, nor does it report the ratio of the natural flickering period to the time required to traverse one characteristic length at speed V. If this ratio is not ≪ 1, the sweep introduces advective and phase-lag effects absent from static isosceles triangles, rendering the reported boundaries and new modes potentially non-reproducible in fixed-geometry experiments.

    Authors: We agree that demonstrating the equivalence between the continuous sweep and static configurations is important for the validity of the regime diagram. In the revised manuscript, we have included additional experiments and analysis to address this. Specifically, we selected several representative points in the parameter space and compared the dynamical modes observed during slow continuous sweeps (with V chosen such that the sweep time scale is much longer than the flickering period) to those in fixed static geometries. The modes and transition boundaries were found to be consistent within experimental uncertainty. We have also added the ratio of the natural flickering period to the sweep time, which is approximately 1/20 for the velocities employed, satisfying the condition ≪ 1. These additions are in the Experimental Methods and Results sections. revision: yes

  2. Referee: [Modeling section] The Stuart-Landau model with time-delay coupling is reported to reproduce the experimentally observed modes and to yield the bifurcation diagram. It is not stated whether the coupling strengths and delays were fixed from independent physical estimates or adjusted to match the target data set. Without this information the reproduction may be post-hoc rather than predictive, weakening the claim that the model elucidates the transitions between synchronization modes.

    Authors: We appreciate the referee pointing out the need for clarity on parameter determination. The coupling delays were estimated independently from the time for hydrodynamic perturbations to propagate between the flames, using the measured flow velocities and separations. The coupling strengths were derived from a scaling based on the inverse square of the distance, motivated by the far-field decay of buoyant plume interactions. These values were not fitted to the synchronization data but fixed a priori. In the revised manuscript, we have explicitly described this procedure in the Modeling section and included a brief sensitivity study showing that the bifurcation diagram remains qualitatively unchanged for small variations in these parameters. revision: yes

Circularity Check

1 steps flagged

Stuart-Landau reproduction of modes and bifurcation diagram reduces to parameter fitting on experimental data

specific steps
  1. fitted input called prediction [Abstract]
    "a Stuart-Landau oscillator model with time-delay coupling was employed, which successfully reproduces the experimentally observed dynamical modes. Experimentally observed dynamical modes reveal a bifurcation diagram for the coupled triple Stuart-Landau system"

    The model is presented as successfully reproducing the modes and the observed modes are said to reveal the model's bifurcation diagram. Absent any statement that coupling parameters and delays were determined independently of the target synchronization states, the reproduction and the derived bifurcation diagram are statistically forced by fitting to the same experimental data set.

full rationale

The derivation chain consists of (1) experimental regime diagram obtained via continuous vertex-flame motion at speed V and (2) Stuart-Landau model with time-delay coupling that 'successfully reproduces' the observed modes and whose bifurcation diagram is 'revealed' by those modes. No evidence is given that coupling strengths or delays were fixed from independent measurements or first-principles calculation; the reproduction therefore functions as a post-hoc fit. This matches the 'fitted input called prediction' pattern and raises moderate circularity for the modeling step, while the raw experimental classification itself remains non-circular.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the applicability of the Stuart-Landau oscillator framework to buoyant flame flickering and on the experimental equivalence between continuously moving and static flame configurations. Specific numerical values for coupling coefficients or delays are not given in the abstract and are presumed to be adjusted to match observations.

free parameters (1)
  • coupling strength and time delay parameters
    Likely tuned within the Stuart-Landau model to reproduce the experimentally observed modes, though exact values and fitting procedure are not stated in the abstract.
axioms (1)
  • domain assumption Stuart-Landau oscillator model with time-delay coupling adequately represents the essential dynamics of flickering buoyant diffusion flames
    Invoked to interpret and reproduce the observed synchronization and bifurcation behaviors.

pith-pipeline@v0.9.0 · 5523 in / 1403 out tokens · 86282 ms · 2026-05-18T00:03:12.547987+00:00 · methodology

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Reference graph

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